US11644351B2

US11644351B2 - Multiphase flow and salinity meter with dual opposite handed helical resonators

Info

Publication number: US11644351B2
Application number: US17/206,741
Authority: US
Inventors: Muhammad Akram Karimi; Muhammad ARSALAN; Atif SHAMIM
Original assignee: Saudi Arabian Oil Co; King Abdullah University of Science and Technology KAUST
Current assignee: Saudi Arabian Oil Co; King Abdullah University of Science and Technology KAUST
Priority date: 2021-03-19
Filing date: 2021-03-19
Publication date: 2023-05-09
Also published as: SA122430793B1; US20220299348A1

Abstract

A multiphase flow measurement apparatus includes a tubular, a first microwave resonator, a second microwave resonator, and a coplanar waveguide resonator. The tubular includes a wall formed to define an inner bore configured to flow a multiphase fluid. The first microwave resonator has a first helical shape with a first longitudinal length and is configured to generate a first electric field that rotates. The second microwave resonator has a second helical shape with a second longitudinal length different from the first longitudinal length of the first microwave resonator and is configured to generate a second electric field that rotates. The first and second microwave resonators are mutually orthogonal to each other and cooperatively configured to measure a salinity of the multiphase fluid flowing through the inner bore. The coplanar waveguide resonator is configured to generate a third electric field to measure a flow rate of the multiphase fluid.

Description

TECHNICAL FIELD

This disclosure relates to multiphase flow measurement.

BACKGROUND

Production fluid typically comes from wells in the form of a complex mixture of three phases (oil, water, and gas) that are co-mingled together. In some cases, a small quantity of solids (such as sand particles) may also be present in the production fluid. Knowledge of the individual flow rates of the various phases of the production fluid from a producing well can help to facilitate reservoir management, field development, operational control, flow assurance, and production allocation.

SUMMARY

This disclosure describes technologies relating to multiphase flow measurement. Certain aspects of the subject matter described can be implemented as a multiphase flow measurement apparatus. The apparatus includes a tubular, a first microwave resonator, a second microwave resonator, and a coplanar waveguide resonator. The tubular includes a wall formed to define an inner bore configured to flow a multiphase fluid. The first microwave resonator is disposed on an outer circumferential surface of the wall. The first microwave resonator has a first helical shape with a first longitudinal length. The first microwave resonator is configured to generate a first electric field that rotates in the inner bore along the first helical shape of the first microwave resonator. The second microwave resonator is disposed on the outer circumferential surface of the wall. The second microwave resonator has a second helical shape with a second longitudinal length different from the first longitudinal length of the first microwave resonator. The second microwave resonator is configured to generate a second electric field that rotates in the inner bore along the second helical shape of the second microwave resonator. The first and second microwave resonators are mutually orthogonal to each other and cooperatively configured to measure a salinity of the multiphase fluid flowing through the inner bore. The coplanar waveguide resonator is disposed on the outer circumferential surface of the wall. The coplanar waveguide resonator is configured to generate a third electric field to measure a flow rate of the multiphase fluid flowing through the inner bore.

This, and other aspects, can include one or more of the following features.

In some implementations, the coplanar waveguide resonator is a first coplanar waveguide resonator. In some implementations, the apparatus includes a second coplanar waveguide resonator disposed on the outer circumferential surface of the wall. In some implementations, the second coplanar waveguide resonator is configured to generate a fourth electric field. In some implementations, the first and second coplanar waveguide resonators are cooperatively configured to measure the flow rate and a dielectric loss of the multiphase fluid flowing through the inner bore.

In some implementations, the first and second microwave resonators are disposed on the outer circumferential surface of the wall between the first and second coplanar waveguide resonators.

In some implementations, the apparatus includes a Venturi tube including a convergent section having a cross-sectional area that is smaller than a cross-sectional area of the inner bore. In some implementations, an outlet of the Venturi tube is coupled to an inlet of the tubular. In some implementations, the apparatus includes a differential pressure sensor fluidically coupled to the Venturi tube upstream and downstream of the convergent section. In some implementations, the differential pressure sensor is configured to measure a pressure drop of the multiphase fluid through the convergent section. In some implementations, the first coplanar waveguide resonator, the second coplanar waveguide resonator, and the differential pressure sensor are cooperatively configured to measure the flow rate of the multiphase fluid flowing through the inner bore. In some implementations, the apparatus includes a temperature sensor coupled to the tubular. In some implementations, the temperature sensor is configured to measure a temperature of the multiphase fluid. In some implementations, the first coplanar waveguide resonator, the second coplanar waveguide resonator, the differential pressure sensor, and the temperature sensor are cooperatively configured to measure the flow rate and the salinity of the multiphase fluid flowing through the inner bore.

In some implementations, the first microwave resonator is configured to generate the first electric field, such that the first electric field makes at least a 360 degree rotation in the inner bore along the first helical shape of the first microwave resonator. In some implementations, the second microwave resonator is configured to generate the second electric field, such that the second electric field makes at least a 360 degree rotation in the inner bore along the second helical shape of the second microwave resonator.

Certain aspects of the subject matter described can be implemented as a multiphase flow measurement apparatus. The apparatus includes a tubular, a first microwave resonator, a second microwave resonator, and a coplanar waveguide resonator. The first microwave resonator is disposed on an exterior of the apparatus. The first microwave resonator has a first helical shape with a first longitudinal length and is configured to generate a first electric field that rotates around the exterior of the apparatus along the first helical shape of the first microwave resonator. The second microwave resonator is disposed on the exterior of the apparatus. The second microwave resonator has a second helical shape with a second longitudinal length different from the first longitudinal length of the first microwave resonator. The second microwave resonator is configured to generate a second electric field that rotates around the exterior of the apparatus along the second helical shape of the second microwave resonator. The first and second microwave resonators are mutually orthogonal to each other and cooperatively configured to measure a salinity of a multiphase fluid flowing across the exterior of the apparatus. The coplanar waveguide resonator is disposed on an exterior of the tubular. The coplanar waveguide resonator is configured to generate a third electric field to measure a flow rate of the multiphase fluid flowing across the exterior of the tubular.

This, and other aspects, can include one or more of the following features.

In some implementations, the first and second microwave resonators are disposed on and wrap around the exterior of the tubular.

In some implementations, the coplanar waveguide resonator is a first coplanar waveguide resonator. In some implementations, the apparatus includes a second coplanar waveguide resonator disposed on the exterior of the tubular and configured to generate a fourth electric field. In some implementations, the first and second coplanar waveguide resonators are cooperatively configured to measure the flow rate and a dielectric loss of the multiphase fluid flowing across the exterior of the apparatus. In some implementations, the first and second microwave resonators are disposed on the exterior of the tubular between the first and second coplanar waveguide resonators.

In some implementations, the apparatus includes a first conical end and a second conical end, wherein the first conical end and the second conical end are coupled to the tubular at opposite ends of the tubular. In some implementations, the first microwave resonator is disposed on and wraps around an exterior of the first conical end. In some implementations, the second microwave resonator is disposed on and wraps around an exterior of the second conical end. In some implementations, the first microwave resonator is configured to generate the first electric field, such that the first electric field makes at least a 360 degree rotation around the first conical end along the first helical shape of the first microwave resonator. In some implementations, the second microwave resonator is configured to generate the second electric field, such that the second electric field makes at least a 360 degree rotation around the second conical end along the second helical shape of the second microwave resonator.

Certain aspects of the subject matter described can be implemented as a method. A multiphase fluid is flowed to contact an apparatus. The apparatus includes a tubular, a first microwave resonator, a second microwave resonator, and a coplanar waveguide resonator. The first microwave resonator has a first helical shape with a first longitudinal length. The second microwave resonator has a second helical shape with a second longitudinal length. The first and second microwave resonators are mutually orthogonal to each other. The coplanar waveguide resonator is disposed on an exterior of the tubular. A first electric field is generated by the first microwave resonator. The first electric field rotates along the first helical shape of the first microwave resonator. A second electric field is generated by the second microwave resonator. The second electric field that rotates along the second helical shape of the second microwave resonator. A third electric field is generated by the coplanar waveguide resonator. A fluid characteristic of the multiphase fluid is determined in response to generating the first, second, and third electric fields. The fluid characteristics includes at least one of flow rate, salinity, or phase fraction.

This, and other aspects, can include one or more of the following features.

In some implementations, the first electric field makes at least a 360 degree rotation along the first helical shape of the first microwave resonator. In some implementations, the second electric field makes at least a 360 degree rotation along the second helical shape of the second microwave resonator.

In some implementations, the apparatus includes a first conical end and a second conical end. In some implementations, the first and second conical ends are coupled to the tubular at opposite ends of the tubular. In some implementations, the first microwave resonator is disposed on and wraps around an exterior of the first conical end. In some implementations, the second microwave resonator is disposed on and wraps around an exterior of the second conical end.

In some implementations, the first and second microwave resonators are disposed on the exterior of the tubular. In some implementations, flowing the multiphase fluid to contact the apparatus includes flowing the multiphase fluid through an inner bore of the tubular.

In some implementations, the method includes generating a fourth electric field by a second coplanar waveguide resonator. In some implementations, the method includes determining a dielectric loss of the multiphase fluid in response to generating the third and fourth electric fields.

The details of one or more implementations of the subject matter of this disclosure are set forth in the accompanying drawings and the description. Other features, aspects, and advantages of the subject matter will become apparent from the description, the drawings, and the claims.

DESCRIPTION OF DRAWINGS

FIG. 1A is a schematic diagram of an example apparatus for multiphase flow measurement in which a multiphase fluid flows through the apparatus.

FIG. 1B is a schematic diagram of an example apparatus for multiphase flow measurement in which a multiphase fluid flows through the apparatus.

FIG. 2 is a schematic diagram of an example apparatus for multiphase flow measurement in which a multiphase fluid flows around an exterior of the apparatus.

FIG. 3 is a schematic diagram of an example apparatus for multiphase flow measurement in which a multiphase fluid flows around an exterior of the apparatus.

FIG. 4 is a flow chart of an example method for multiphase flow measurement.

FIG. 5A is a plot showing the effect of salinity on the dielectric constant of brines.

FIG. 5B is a plot showing response signals of two resonators having different frequencies to an oil/water medium.

FIG. 5C is a plot showing the effect of salinity on resonance separation in brines.

DETAILED DESCRIPTION

This disclosure describes multiphase flow measurement. A multiphase flow measurement apparatus includes a microwave resonator and a coplanar waveguide resonator. Both the microwave resonator and the coplanar waveguide resonator can be printed on an exterior surface of a non-metallic material. The apparatus can include multiple microwave resonators with different longitudinal lengths, such that the microwave resonators have different resonant frequencies. The apparatus can include multiple coplanar waveguide resonators. The microwave resonator(s) and the coplanar waveguide resonator(s) generate electric fields and are cooperatively configured to determine properties of a multiphase fluid. In some cases, the multiphase fluid flows through an inner bore of the apparatus. In some cases, the multiphase fluid flows across an exterior of the apparatus. In some cases, data from the microwave resonator(s) and coplanar waveguide resonator(s) are correlated with process data, such as pressure and/or temperature of the multiphase fluid.

The subject matter described in this disclosure can be implemented in particular implementations, so as to realize one or more of the following advantages. The apparatuses and methods described utilize electric fields having frequencies in the microwave spectrum, which can be safer in comparison to measurements that utilize radioactive sources to measure multiphase flow. The apparatuses described are compact in size, which can be useful in space-restricted environments. For example, the apparatuses can be implemented for multiphase fluid flow measurement in pipes having a diameter of 4 inches or larger. The apparatuses and methods described can be implemented to determine properties of a multiphase fluid without requiring mixing of the multiphase fluid prior to measurement. The apparatuses described are not sensitive to orientation and can be easily installed to existing equipment. In some implementations, the apparatus is non-intrusive and does not introduce any obstruction to the flow area of the multiphase fluid. The apparatuses and methods described implement helical T-resonator whose resonant frequency can be adjusted by increasing or decreasing a length of the resonator, for example, by adjusting the manner in which the resonator is printed on a surface of the apparatus. By allowing for ease of resonant frequency adjustment, the apparatuses and methods described can be implemented to measure dielectric properties at different frequencies to form a basis for multiphase flow measurements, such as water-cut ratio and gas volume fraction. In some cases, the resonant frequency of the printed helical T-resonator can be easily adjusted even after fabrication. In contrast, such post-fabrication adjustments to resonant frequency can be difficult for conventional resonators, such as cavity type resonators.

FIG. 1A is a schematic diagram of an example apparatus 100 for multiphase flow measurement in which a multiphase fluid 150 flows through the apparatus 100. The multiphase fluid 150 is a fluid that includes multiple phases of matter. For example, the multiphase fluid 150 includes a liquid phase (such as oil) and a gas phase. For example, the multiphase fluid 150 includes multiple liquid phases (such as an aqueous fluid and oil). For example, the multiphase fluid 150 includes multiple liquid phases and a gas phase. The apparatus 100 includes a tubular 101 that includes a wall 101 a that defines an inner bore configured to flow the multiphase fluid 150. The apparatus 100 includes a first microwave resonator 103 a, a second microwave resonator 103 b, and a coplanar waveguide resonator 105 a. In some implementations, the first and

second microwave resonators

103 a, 103 b are printed on the wall 101 a of the tubular 101. In some implementations, the coplanar waveguide resonator 105 a is printed on the wall 101 a of the tubular 101. In some implementations, the tubular 101 is made of a non-metallic material. For example, the tubular 101 is made of a polymeric material, such as polyether ether ketone (PEEK). For example, the tubular 101 is made of a composite material. In such implementations, the tubular 101 itself does not function as a resonating material and remains unaffected by electric fields generated by other components of the apparatus 100, such as the microwave resonators (103 a, 103 b) and the coplanar waveguide resonator 105 a.

The first microwave resonator 103 a and the second microwave resonator 103 b can be substantially similar. The first and

second microwave resonators

103 a, 103 b are disposed on an outer circumferential surface of the wall 101 a of the tubular 101. For example, the first and

second microwave resonators

103 a, 103 b are spiral T-resonators. The first microwave resonator 103 a has a first helical shape with a first longitudinal length (l₁). The second microwave resonator 103 b has a second helical shape with a second longitudinal length (l₂) that is different from the first longitudinal length (l₁). For example, the second longitudinal length (l₂) is shorter or longer than the first longitudinal length (l₁). In some implementations, each of the first and second longitudinal lengths (l₁, l₂) are in a range of from about 4 inches (in) to about 10 in.

Because the first and

second microwave resonators

103 a, 103 b have different longitudinal lengths, they have different resonant frequencies. The first microwave resonator 103 a is configured to generate a first electric field that rotates in the inner bore of the tubular 101 along the first helical shape of the first microwave resonator 103 a. The first electric field has a frequency in the microwave spectrum. In some implementations, the first electric field has a frequency in a range of from 50 megahertz (MHz) to 300 gigahertz (GHz), from 50 MHz to 500 MHz, or from 300 MHz to 500 MHz. The second microwave resonator 103 b is configured to generate a second electric field that rotates in the inner bore of the tubular 101 along the second helical shape of the second microwave resonator 103 b. The second electric field has a frequency in the microwave spectrum. In some implementations, the first electric field has a frequency in a range of from 50 MHz to 300 gigahertz GHz, from 50 MHz to 500 MHz, or from 300 MHz to 500 MHz. The first and

second microwave resonators

103 a, 103 b are mutually orthogonal to each other. Therefore, the first and second electric fields generated by the first and

second microwave resonators

103 a, 103 b, respectively, are also mutually orthogonal to each other.

The first and

second microwave resonators

103 a, 103 b are cooperatively configured to measure a salinity of the multiphase fluid 150 flowing through the inner bore of the tubular 101. For example, the first and

second microwave resonators

103 a, 103 b generate the first and second electric fields, respectively, which excite molecules in the multiphase fluid 150 at different frequencies, and the slope of a measured dielectric loss can be determined to measure the salinity of the multiphase fluid 150. In some implementations, the first and

second microwave resonators

103 a, 103 b are cooperatively configured to measure a flow rate (for example, volumetric flow rate or mass flow rate) of the multiphase fluid 150 flowing through the inner bore of the tubular 101. In some implementations, the first and

second microwave resonators

103 a, 103 b are cooperatively configured to measure phase fractions of the different phases (for example, oil phase, aqueous phase, and vapor phase) of the multiphase fluid 150 flowing through the inner bore of the tubular 101. In some implementations, the first electric field generated by the first microwave resonator 103 a makes at least a 360 degree rotation (one full revolution) in the inner bore along the first helical shape of the first microwave resonator 103 a. In some implementations, the second electric field generated by the second microwave resonator 103 b makes at least a 360 degree rotation (one full revolution) in the inner bore along the second helical shape of the second microwave resonator 103 b.

In some implementations, the longitudinal lengths (l₁, l₂) of the first and

second microwave resonators

103 a, 103 b allow them to act as low-pass filters. As a result, quick changes (for example, a change with a timescale on the order of 5 to 10 milliseconds (ms)) in the multiphase fluid 150 (for example, salinity or velocity) can be averaged over a time period (for example, in a range of from about 25 ms to about 50 ms). For example, a multiphase fluid can have turbulent flow, and its geometric distribution within a cross-section of a tubular may quickly change. Such fluctuating variations in the multiphase fluid can be averaged over a length of the apparatus 100 (for example, the length of the first and

second microwave resonators

103 a, 103 b), and turbulence appearance in the readout circuitry can be slower.

The apparatus 100 includes a ground conductor, such as a ring-shaped ground conductor. In some implementations, each of the

microwave resonators

103 a, 103 b is paired with a respective helical ground conductor. Mutual rotation of the

resonators

103 a, 103 b and helical ground conductors can facilitate rotation of the electric fields.

The coplanar waveguide resonator 105 a is disposed on the outer circumferential surface of the wall 101 a. The coplanar waveguide resonator 105 a can be, for example, a ring resonator. The coplanar waveguide resonator 105 a is configured to generate a third electric field to measure a flow rate of the multiphase fluid 150, for example, flowing through the inner bore of the tubular 101. The third electric field has a frequency in the microwave spectrum. In some implementations, the third electric field has a frequency in a range of from about 250 MHz to about 1000 MHz. In some implementations, the third electric field generated by the coplanar waveguide resonator 105 a has a shallower reach (that is, electric field penetration) into a substrate in comparison to the first and second electric fields generated by the first and

second microwave resonators

103 a, 103 b, respectively. In some implementations, the coplanar waveguide resonator 105 a is configured to measure the salinity of the multiphase fluid 150. For example, the coplanar waveguide resonator 105 a can be configured to measure the salinity of the multiphase fluid 150 flowing in an annular flow regime, in which liquid forms a continuous film along an inner circumferential surface of the wall 101 a of the tubular 101. Varying wall thicknesses of the wall 101 a of the tubular 101 can be accommodated by adjusting a gap between signal and ground conductors of the coplanar waveguide resonator 105 a, such that the third electric field generated by the coplanar waveguide resonator 105 a has sufficient reach, for example, to detect the liquid film formed on the inner circumferential surface of the wall 101 a of the tubular 101 and remain unaffected by gas flowing further away from the wall 101 a and closer to the center of the tubular 101. In some implementations, the coplanar waveguide resonator 105 a is made of the same material as the first and

second microwave resonators

103 a, 103 b.

In some implementations, the apparatus 100 includes a second coplanar waveguide resonator 105 b. The second coplanar waveguide resonator 105 b can be, for example, a ring resonator. Similar to the first waveguide resonator 105 a, the second coplanar waveguide resonator 105 b can be disposed on the outer circumferential surface of the wall 101 a. The second coplanar waveguide resonator 105 b can be configured to generate a fourth electric field similar to the third electric field generated by the coplanar waveguide resonator 105 a. The fourth electric field can have a frequency in the microwave spectrum. In some implementations, the fourth electric field has a frequency in a range of from about 250 MHz to about 1000 MHz. In some implementations, the fourth electric field generated by the second coplanar waveguide resonator 105 b has a shallower reach (that is, electric field penetration) into a substrate in comparison to the first and second electric fields generated by the first and

second microwave resonators

103 a, 103 b, respectively. In some implementations, the first and second

coplanar waveguide resonators

105 a, 105 b are cooperatively configured to measure the flow rate and a dielectric loss of the multiphase fluid 150 flowing through the inner bore of the tubular 101. The dielectric loss of the multiphase fluid 150 measured by the first and second

coplanar waveguide resonators

105 a, 105 b can be correlated to the salinity of the multiphase fluid 150. In some implementations, the first and

second microwave resonators

103 a, 103 b are disposed on the outer circumferential surface of the wall 101 a between the first and second

coplanar waveguide resonators

105 a, 105 b. In some implementations, the apparatus 100 includes additional coplanar waveguide resonators (similar to 105 a, 105 b) that can be used to measure flow rate in flow regimes other than the annular flow regime (for example, turbulent regime). In some implementations, the second coplanar waveguide resonator 105 b is made of the same material as the first and

second microwave resonators

103 a, 103 b. The

coplanar waveguide resonators

105 a, 105 b and the

microwave resonators

103 a, 103 b can all be types of microwave resonators that function differently based on shape and size.

FIG. 1B is a schematic diagram of an apparatus 190 for multiphase flow measurement in which a multiphase fluid 150 flows through the apparatus 190. The apparatus 190 can be substantially similar to the apparatus 100. For example, apparatus 190 can include component(s) of apparatus 100. In some implementations, the apparatus 190 includes a Venturi tube 110. In some implementations, the Venturi tube 110 includes a convergent section 110 a having a cross-sectional area that is smaller than a cross-sectional area of the inner bore of the tubing 101. In some implementations, an outlet 110 b of the Venturi tube 110 is coupled to an inlet 101 b of the tubular 101. In some implementations, the apparatus 190 includes a differential pressure sensor 111 fluidically coupled to the Venturi tube 110 upstream and downstream of the convergent section 110 a. The differential pressure sensor 111 is configured to measure a pressure drop of the multiphase fluid 150 through the convergent section 110 a. In some implementations, the coplanar waveguide resonator 105 a, the second coplanar waveguide resonator 105 b, and the differential pressure sensor 111 are cooperatively configured to measure the flow rate of the multiphase fluid 150, for example, flowing through the inner bore of the tubular 101. For example, the flow rate determined by the first and second

coplanar waveguide resonators

105 a, 105 b can be correlated to the pressure drop measured by the differential pressure sensor 111 to more accurately calculate the flow rate of the multiphase fluid 150.

In some implementations, the apparatus 190 includes a temperature sensor 120. In some implementations, the temperature sensor 120 is coupled to an outlet 101 c of the tubular 101. The temperature sensor 120 is configured to measure a temperature of the multiphase fluid 150, for example, flowing through the inner bore of the tubular 101. In some implementations, the coplanar waveguide resonator 105 a, the second coplanar waveguide resonator 105 b, the differential pressure sensor 111, and the temperature sensor 120 are cooperatively configured to measure the flow rate and the salinity of the multiphase fluid 150, for example, flowing through the inner bore of the tubular 101. In some implementations, the temperature sensor 120 is an inline temperature sensor.

FIG. 2 is a schematic diagram of an example apparatus 200 for multiphase flow measurement in which a multiphase fluid 150 flows around an exterior of the apparatus 200. The apparatus 200 is configured to be disposed within a pipe that flows a multiphase fluid (such as the multiphase fluid 150). The multiphase fluid 150 flows across an exterior of the apparatus 200. The apparatus 200 can be substantially similar to the apparatus 100. For example, apparatus 200 can include component(s) of apparatus 100.

The apparatus 200 includes a tubular 201. The apparatus 200 includes a first conical end 201 a and a second conical end 201 b. The first and second conical ends 201 a, 201 b are coupled to the tubular 201 at opposite ends of the tubular 201. The apparatus 200 includes a first microwave resonator 203 a, a second microwave resonator 203 b, and a coplanar waveguide resonator 205 a. In some implementations, the first and

second microwave resonators

203 a, 203 b are printed on an exterior of the tubular 201. In some implementations, the coplanar waveguide resonator 205 a is printed on the exterior of the tubular 201. In some implementations, the tubular 201 is made of a non-metallic material. For example, the tubular 201 is made of a polymeric material, such as polyether ether ketone (PEEK). For example, the tubular 201 is made of a composite material. In such implementations, the tubular 201 itself does not function as a resonating material and remains unaffected by electric fields generated by other components of the apparatus 200, such as the microwave resonators (203 a, 203 b) and the coplanar waveguide resonator 205 a.

The first and

second microwave resonators

203 a, 203 b can be substantially similar to the first and

second microwave resonators

103 a, 103 b. The first microwave resonator 203 a and the second microwave resonator 203 b can be substantially similar. In some implementations, the first and

second microwave resonators

203 a, 203 b are disposed on an outer circumferential surface of the tubular 201. The first microwave resonator 203 a has a first helical shape with a first longitudinal length (l₁). The second microwave resonator 203 b has a second helical shape with a second longitudinal length (l₂) that is different from the first longitudinal length (l₁). For example, the second longitudinal length (l₂) is shorter or longer than the first longitudinal length (l₁). Because the first and

second microwave resonators

203 a, 203 b have different longitudinal lengths, they have different resonant frequencies. The first microwave resonator 203 a is configured to generate a first electric field that rotates around the exterior of the tubular 201 along the first helical shape of the first microwave resonator 203 a. The first electric field has a frequency in the microwave spectrum. The second microwave resonator 203 b is configured to generate a second electric field that rotates around the exterior of the tubular 201 along the second helical shape of the second microwave resonator 203 b. The second electric field has a frequency in the microwave spectrum. The first and

second microwave resonators

203 a, 203 b are mutually orthogonal to each other. Therefore, the first and second electric fields generated by the first and

second microwave resonators

203 a, 203 b, respectively, are also mutually orthogonal to each other.

The first and

second microwave resonators

203 a, 203 b are cooperatively configured to measure a salinity of the multiphase fluid 150 flowing across the exterior of the tubular 201. For example, the first and

second microwave resonators

203 a, 203 b generate the first and second electric fields, respectively, which excite molecules in the multiphase fluid 150 at different frequencies, and the slope of a measured dielectric loss can be determined to measure the salinity of the multiphase fluid 150. In some implementations, the first and

second microwave resonators

203 a, 203 b are cooperatively configured to measure a flow rate (for example, volumetric flow rate or mass flow rate) of the multiphase fluid 150 flowing across the exterior of the tubular 201. In some implementations, the first and

second microwave resonators

203 a, 203 b are cooperatively configured to measure phase fractions of the different phases (for example, oil phase, aqueous phase, and vapor phase) of the multiphase fluid 150 flowing across the exterior of the tubular 101. In some implementations, the first electric field generated by the first microwave resonator 203 a makes at least a 360 degree rotation (one full revolution) around the exterior of the tubular 201 along the first helical shape of the first microwave resonator 203 a. In some implementations, the second electric field generated by the second microwave resonator 203 b makes at least a 360 degree rotation (one full revolution) around the exterior of the tubular 201 along the second helical shape of the second microwave resonator 203 b.

The coplanar waveguide resonator 205 a can be substantially similar to the coplanar waveguide resonator 105 a. The coplanar waveguide resonator 205 a is disposed on the outer circumferential surface of the tubular 201. The coplanar waveguide resonator 205 a is configured to generate a third electric field to measure a flow rate of the multiphase fluid 150, for example, flowing across the exterior of the tubular 201. The third electric field has a frequency in the microwave spectrum. In some implementations, the coplanar waveguide resonator 205 a is configured to measure the salinity of the multiphase fluid 150.

In some implementations, the apparatus 200 includes a second coplanar waveguide resonator 205 b. Similar to the first waveguide resonator 205 a, the second coplanar waveguide resonator 205 b can be disposed on the outer circumferential surface of the tubular 201. The second coplanar waveguide resonator 205 b can be configured to generate a fourth electric field similar to the third electric field generated by the coplanar waveguide resonator 205 a. The fourth electric field can have a frequency in the microwave spectrum. In some implementations, the first and second

coplanar waveguide resonators

205 a, 205 b are cooperatively configured to measure the flow rate and a dielectric loss of the multiphase fluid 150 flowing across the exterior of the tubular 201. In some implementations, the first and

second microwave resonators

203 a, 203 b are disposed on the outer circumferential surface of the tubular 201 between the first and second

coplanar waveguide resonators

205 a, 205 b. In some implementations, the apparatus 200 includes additional coplanar waveguide resonators (similar to 205 a, 205 b) that can be used to measure flow rate in flow regimes other than the annular flow regime (for example, turbulent regime).

FIG. 3 is a schematic diagram of an example apparatus 300 for multiphase flow measurement in which a multiphase fluid 150 flows around an exterior of the apparatus 300. The apparatus 300 is configured to be disposed within a pipe that flows a multiphase fluid (such as the multiphase fluid 150). The multiphase fluid 150 flows across an exterior of the apparatus 300. The apparatus 300 can be substantially similar to the apparatus 100 and/or apparatus 200. For example, apparatus 300 can include component(s) of apparatus 100 and/or apparatus 200. In some cases, apparatus 300 is the most compact in size in comparison to

apparatuses

100 and 200.

The apparatus 300 includes a tubular 301. The apparatus 300 includes a first conical end 301 a and a second conical end 301 b. The first and second conical ends 301 a, 301 b are coupled to the tubular 301 at opposite ends of the tubular 301. The apparatus 300 includes a first microwave resonator 303 a, a second microwave resonator 303 b, and a coplanar waveguide resonator 305 a. In some implementations, the first microwave resonator 303 a is printed on an exterior of the first conical end 301 a. In some implementations, the second microwave resonator 303 b is printed on an exterior of the second conical end 301 b. In some implementations, the coplanar waveguide resonator 305 a is printed on the exterior of the tubular 301. In some implementations, the tubular 301 is made of a non-metallic material. For example, the tubular 301 is made of a polymeric material, such as polyether ether ketone (PEEK). For example, the tubular 301 is made of a composite material. In such implementations, the tubular 301 itself does not function as a resonating material and remains unaffected by electric fields generated by other components of the apparatus 300, such as the microwave resonators (303 a, 303 b) and the coplanar waveguide resonator 305 a.

Electrical components can be housed within the apparatus 300. For example, the first conical end 301 a, the second conical end 301 b, and the tubular 301 form a housing within which electrical components can be disposed and protected from exposure to the multiphase fluid 150. The apparatus 300 can be supported, for example, by pipes coupled at opposite ends of the apparatus 300. The pipes can provide structural support for the apparatus 300 and can also route wiring to electrical components housed within the apparatus 300.

The first and

second microwave resonators

303 a, 303 b can be substantially similar to the first and

second microwave resonators

103 a, 103 b. The first microwave resonator 303 a and the second microwave resonator 303 b can be substantially similar. In some implementations, the first microwave resonator 303 a is disposed on an exterior of the first conical end 301 a. In some implementations, the first microwave resonator 303 a wraps around the exterior of the first conical end 301 a. The first microwave resonator 303 a has a first helical shape with a first longitudinal length (l₁). The second microwave resonator 303 b has a second helical shape with a second longitudinal length (l₂) that is different from the first longitudinal length (l₁). For example, the second longitudinal length (l₂) is shorter or longer than the first longitudinal length (l₁). Because the first and

second microwave resonators

303 a, 303 b have different longitudinal lengths, they have different resonant frequencies. The first microwave resonator 303 a is configured to generate a first electric field that rotates around the exterior of the first conical end 301 a along the first helical shape of the first microwave resonator 303 a. The first electric field has a frequency in the microwave spectrum. The second microwave resonator 303 b is configured to generate a second electric field that rotates around the exterior of the second conical end 301 b along the second helical shape of the second microwave resonator 303 b. The second electric field has a frequency in the microwave spectrum. The first and

second microwave resonators

303 a, 303 b are mutually orthogonal to each other. Therefore, the first and second electric fields generated by the first and

second microwave resonators

303 a, 303 b, respectively, are also mutually orthogonal to each other.

The first and

second microwave resonators

303 a, 303 b are cooperatively configured to measure a salinity of the multiphase fluid 150 flowing across the exterior of the apparatus 300 (for example, the exterior of the first and second conical ends 301 a, 301 b). For example, the first and

second microwave resonators

303 a, 303 b generate the first and second electric fields, respectively, which excite molecules in the multiphase fluid 150 at different frequencies, and the slope of a measured dielectric loss can be determined to measure the salinity of the multiphase fluid 150. In some implementations, the first and second microwave resonators 303 a, 2303 b are cooperatively configured to measure a flow rate (for example, volumetric flow rate or mass flow rate) of the multiphase fluid 150 flowing across the exterior of the apparatus 300. In some implementations, the first and

second microwave resonators

303 a, 303 b are cooperatively configured to measure phase fractions of the different phases (for example, oil phase, aqueous phase, and vapor phase) of the multiphase fluid 150 flowing across the exterior of the apparatus 300. In some implementations, the first electric field generated by the first microwave resonator 303 a makes at least a 360 degree rotation (one full revolution) around the exterior of the first conical end 301 a along the first helical shape of the first microwave resonator 303 a. In some implementations, the second electric field generated by the second microwave resonator 203 b makes at least a 360 degree rotation (one full revolution) around the exterior of the second conical end 301 b along the second helical shape of the second microwave resonator 303 b.

The coplanar waveguide resonator 305 a can be substantially similar to the coplanar waveguide resonator 105 a. The coplanar waveguide resonator 305 a is disposed on the outer circumferential surface of the tubular 301. The coplanar waveguide resonator 305 a is configured to generate a third electric field to measure a flow rate of the multiphase fluid 150, for example, flowing across the exterior of the apparatus 300 (for example, the exterior of the tubular 301). The third electric field has a frequency in the microwave spectrum. In some implementations, the coplanar waveguide resonator 305 a is configured to measure the salinity of the multiphase fluid 150.

FIG. 4 is a flow chart of an example method 400 for multiphase flow measurement. Any of the

apparatuses

100, 200, or 300 can be used to implement the method 400. For clarity, steps 402, 404, 406, 408, and 410 are described in relation to apparatus 100 even though

apparatuses

200 and 300 can be used to implement these steps as well. At step 402, a multiphase fluid (such as the multiphase fluid 150) is flowed to contact the apparatus 100. In some implementations, the multiphase fluid 150 is flowed through the inner bore of the tubular 101.

At step 404, a first electric field is generated by the first microwave resonator 103 a. The first electric field generated by the first microwave resonator 103 a at step 404 rotates along the first helical shape of the first microwave resonator 103 a. In some implementations, the first electric field generated by the first microwave resonator 103 a at step 404 makes at least a 360 degree rotation along the first helical shape of the first microwave resonator 103 a. The first electric field generated by the first microwave resonator 103 a at step 404 can have frequency in the microwave spectrum. In some implementations, the first microwave resonator 103 a is disposed on the exterior of the tubular 101. In some implementations, the first electric field generated by the first microwave resonator 103 a at step 404 rotates in the inner bore of the tubular 101.

At step 406, a second electric field is generated by the second microwave resonator 103 b. The second electric field generated by the second microwave resonator 103 b at step 406 rotates along the second helical shape of the second microwave resonator 103 b. In some implementations, the second electric field generated by the second microwave resonator 103 b at step 406 makes at least a 360 degree rotation along the second helical shape of the second microwave resonator 103 b. The second electric field generated by the second microwave resonator 103 b at step 404 can have a frequency in the microwave spectrum. In some implementations, the second microwave resonator 103 b is disposed on the exterior of the tubular 101. In some implementations, the second electric field generated by the second microwave resonator 103 b at step 406 rotates in the inner bore of the tubular 101.

At step 408, a third electric field is generated by the coplanar waveguide resonator 105 a. The third electric field generated by the coplanar waveguide resonator 105 a at step 408 can have a frequency in the microwave spectrum. In some implementations, a fourth electric field is generated by the second coplanar waveguide resonator 105 b. The fourth electric field generated by the second coplanar waveguide resonator 105 b can have a frequency in the microwave spectrum.

At step 410, a fluid characteristic of the multiphase fluid 150 is determined in response to generating the first, second, and third electric fields at

steps

404, 406, and 408, respectively. The fluid characteristic includes at least one of flow rate, salinity, or phase fraction (such as water cut or gas volume fraction). In some implementations, a dielectric loss of the multiphase fluid 150 is determined in response to generating the third and fourth electric fields.

Examples

FIG. 5A is a plot 500 showing the effect of salinity on the dielectric constant of brines. The brines had salinity levels ranging from 5,000 parts per million (ppm) to 200,000 ppm. The dielectric constant (also referred as relative permittivity) of the brines were measured over a range of frequencies. As shown in FIG. 5A, dielectric constant (er′) dispersion increases as salinity increases, and the dispersion of the saltiest brine (200,000 ppm) was greatest. Therefore, dielectric constant dispersion can be correlated to salinity level. The

apparatuses

100, 200, and 300 can be used to measure a dielectric constant dispersion of the multiphase fluid 150, which can then be used to determine the salinity of the multiphase fluid 150. The slope of the dielectric constant (er′) curve also varies with respect to frequency. By using resonators working at different frequencies, the salinity of the multiphase fluid 150 can be measured without needing to take a sample of the fluid 150 and analyzing the sample, for example, in a lab. Further, by using resonators working at different frequencies, the apparatus can auto-calibrate and therefore eliminate the need for frequent recalibrations. In some cases, the dielectric constant measurements at different frequencies can be used to estimate other unknown characteristics, such as water cut ratio or gas volume fraction of the multiphase fluid 150.

FIG. 5B is a plot 510 showing response signals of two resonators having different frequencies to an oil/water medium. Resonator 1 was labeled high frequency (HF), and Resonator 2 was labeled low frequency (LF). The HF Resonator 1 measured dielectric properties of the multiphase fluid at a higher frequency in comparison to the LF Resonator 2. S₂₁(y-axis) is a measure of the signal coming out of the output port relative to the stimulus entering the input port of the respective resonator. The difference in the two curves (for example, the separation or difference between the resonant frequencies) can define a slope and can be characteristic of a certain salinity level (for example, shown in FIG. 5C). Therefore, the difference in the two curves can be correlated to the salinity of the aqueous phase of a multiphase fluid 150, the water cut ratio of the multiphase fluid 150, the gas volume fraction of the multiphase fluid 150, or a combination of these.

FIG. 5C is a plot 520 showing the effect of salinity on resonance separation in brines. WC (%) is water cut percentage. As shown in FIG. 5C, resonance separation increases as salinity increases, which is consistent with the results shown in FIG. 5A (dispersion of dielectric constant). Therefore, resonance separation (similar to dielectric constant dispersion) can be correlated to salinity level. The

apparatuses

100, 200, and 300 can be used to measure a resonance separation of the multiphase fluid 150, which can then be used to determine the salinity of the multiphase fluid 150. The resonance separation can also be correlated to the water cut ratio of the multiphase fluid 150 and/or the gas volume fraction of the multiphase fluid 150.

While this specification contains many specific implementation details, these should not be construed as limitations on the scope of what may be claimed, but rather as descriptions of features that may be specific to particular implementations. Certain features that are described in this specification in the context of separate implementations can also be implemented, in combination, in a single implementation. Conversely, various features that are described in the context of a single implementation can also be implemented in multiple implementations, separately, or in any sub-combination. Moreover, although previously described features may be described as acting in certain combinations and even initially claimed as such, one or more features from a claimed combination can, in some cases, be excised from the combination, and the claimed combination may be directed to a sub-combination or variation of a sub-combination.

As used in this disclosure, the terms “a,” “an,” or “the” are used to include one or more than one unless the context clearly dictates otherwise. The term “or” is used to refer to a nonexclusive “or” unless otherwise indicated. The statement “at least one of A and B” has the same meaning as “A, B, or A and B.” In addition, it is to be understood that the phraseology or terminology employed in this disclosure, and not otherwise defined, is for the purpose of description only and not of limitation. Any use of section headings is intended to aid reading of the document and is not to be interpreted as limiting; information that is relevant to a section heading may occur within or outside of that particular section.

As used in this disclosure, the term “about” or “approximately” can allow for a degree of variability in a value or range, for example, within 10%, within 5%, or within 1% of a stated value or of a stated limit of a range.

As used in this disclosure, the term “substantially” refers to a majority of, or mostly, as in at least about 50%, 60%, 70%, 80%, 90%, 95%, 96%, 97%, 98%, 99%, 99.5%, 99.9%, 99.99%, or at least about 99.999% or more.

Values expressed in a range format should be interpreted in a flexible manner to include not only the numerical values explicitly recited as the limits of the range, but also to include all the individual numerical values or sub-ranges encompassed within that range as if each numerical value and sub-range is explicitly recited. For example, a range of “0.1% to about 5%” or “0.1% to 5%” should be interpreted to include about 0.1% to about 5%, as well as the individual values (for example, 1%, 2%, 3%, and 4%) and the sub-ranges (for example, 0.1% to 0.5%, 1.1% to 2.2%, 3.3% to 4.4%) within the indicated range. The statement “X to Y” has the same meaning as “about X to about Y,” unless indicated otherwise. Likewise, the statement “X, Y, or Z” has the same meaning as “about X, about Y, or about Z,” unless indicated otherwise.

Particular implementations of the subject matter have been described. Other implementations, alterations, and permutations of the described implementations are within the scope of the following claims as will be apparent to those skilled in the art. While operations are depicted in the drawings or claims in a particular order, this should not be understood as requiring that such operations be performed in the particular order shown or in sequential order, or that all illustrated operations be performed (some operations may be considered optional), to achieve desirable results. In certain circumstances, multitasking or parallel processing (or a combination of multitasking and parallel processing) may be advantageous and performed as deemed appropriate.

Moreover, the separation or integration of various system modules and components in the previously described implementations should not be understood as requiring such separation or integration in all implementations, and it should be understood that the described components and systems can generally be integrated together or packaged into multiple products.

Accordingly, the previously described example implementations do not define or constrain the present disclosure. Other changes, substitutions, and alterations are also possible without departing from the spirit and scope of the present disclosure.

Claims

What is claimed is:

1. A multiphase flow measurement apparatus comprising:

a tubular comprising a wall formed to define an inner bore configured to flow a multiphase fluid;

a first microwave resonator disposed on an outer circumferential surface of the wall, the first microwave resonator having a first helical shape with a first longitudinal length, the first microwave resonator configured to generate a first electric field that rotates in the inner bore along the first helical shape of the first microwave resonator;

a second microwave resonator disposed on the outer circumferential surface of the wall, the second microwave resonator having a second helical shape with a second longitudinal length different from the first longitudinal length of the first microwave resonator, the second microwave resonator configured to generate a second electric field that rotates in the inner bore along the second helical shape of the second microwave resonator, the first and second microwave resonators oppositely handed with respect to each other and cooperatively configured to measure a salinity of the multiphase fluid flowing through the inner bore; and

a coplanar waveguide resonator disposed on the outer circumferential surface of the wall, the coplanar waveguide resonator configured to generate a third electric field to measure a flow rate of the multiphase fluid flowing through the inner bore.

2. The apparatus of claim 1, wherein:

the coplanar waveguide resonator is a first coplanar waveguide resonator;

the apparatus comprises a second coplanar waveguide resonator disposed on the outer circumferential surface of the wall and configured to generate a fourth electric field; and

the first and second coplanar waveguide resonators are cooperatively configured to measure the flow rate and a dielectric loss of the multiphase fluid flowing through the inner bore.

3. The apparatus of claim 2, wherein the first and second microwave resonators are disposed on the outer circumferential surface of the wall between the first and second coplanar waveguide resonators.

4. The apparatus of claim 2, comprising a Venturi tube comprising a convergent section having a cross-sectional area that is smaller than a cross-sectional area of the inner bore, wherein an outlet of the Venturi tube is coupled to an inlet of the tubular.

5. The apparatus of claim 4, comprising a differential pressure sensor fluidically coupled to the Venturi tube upstream and downstream of the convergent section, the differential pressure sensor configured to measure a pressure drop of the multiphase fluid through the convergent section, wherein the first coplanar waveguide resonator, the second coplanar waveguide resonator, and the differential pressure sensor are cooperatively configured to measure the flow rate of the multiphase fluid flowing through the inner bore.

6. The apparatus of claim 5, comprising a temperature sensor coupled to the tubular, the temperature sensor configured to measure a temperature of the multiphase fluid, wherein the first coplanar waveguide resonator, the second coplanar waveguide resonator, the differential pressure sensor, and the temperature sensor are cooperatively configured to measure the flow rate and the salinity of the multiphase fluid flowing through the inner bore.

7. The apparatus of claim 6, wherein:

the first microwave resonator is configured to generate the first electric field, such that the first electric field makes at least a 360 degree rotation in the inner bore along the first helical shape of the first microwave resonator; and

the second microwave resonator is configured to generate the second electric field, such that the second electric field makes at least a 360 degree rotation in the inner bore along the second helical shape of the second microwave resonator.

8. A multiphase flow measurement apparatus comprising:

a tubular;

a first microwave resonator disposed on an exterior of the apparatus, the first microwave resonator having a first helical shape with a first longitudinal length and configured to generate a first electric field that rotates around the exterior of the apparatus along the first helical shape of the first microwave resonator;

a second microwave resonator disposed on the exterior of the apparatus, the second microwave resonator having a second helical shape with a second longitudinal length different from the first longitudinal length of the first microwave resonator, the second microwave resonator configured to generate a second electric field that rotates around the exterior of the apparatus along the second helical shape of the second microwave resonator, the first and second microwave resonators oppositely handed with respect to each other and cooperatively configured to measure a salinity of a multiphase fluid flowing across the exterior of the apparatus; and

a coplanar waveguide resonator disposed on an exterior of the tubular, wherein the coplanar waveguide resonator is configured to generate a third electric field to measure a flow rate of the multiphase fluid flowing across the exterior of the tubular.

9. The apparatus of claim 8, wherein the first and second microwave resonators are disposed on and wrap around the exterior of the tubular.

10. The apparatus of claim 9, wherein:

the coplanar waveguide resonator is a first coplanar waveguide resonator;

the apparatus comprises a second coplanar waveguide resonator disposed on the exterior of the tubular and configured to generate a fourth electric field; and

the first and second coplanar waveguide resonators are cooperatively configured to measure the flow rate and a dielectric loss of the multiphase fluid flowing across the exterior of the apparatus.

11. The apparatus of claim 10, wherein the first and second microwave resonators are disposed on the exterior of the tubular between the first and second coplanar waveguide resonators.

12. The apparatus of claim 8, comprising a first conical end and a second conical end, wherein the first conical end and the second conical end are coupled to the tubular at opposite ends of the tubular.

13. The apparatus of claim 12, wherein the first microwave resonator is disposed on and wraps around an exterior of the first conical end, and the second microwave resonator is disposed on and wraps around an exterior of the second conical end.

14. The apparatus of claim 13, wherein:

the first microwave resonator is configured to generate the first electric field, such that the first electric field makes at least a 360 degree rotation around the first conical end along the first helical shape of the first microwave resonator; and

the second microwave resonator is configured to generate the second electric field, such that the second electric field makes at least a 360 degree rotation around the second conical end along the second helical shape of the second microwave resonator.

15. A method comprising:

flowing a multiphase fluid to contact an apparatus, the apparatus comprising:

a tubular;

a first microwave resonator having a first helical shape with a first longitudinal length;

a second microwave resonator having a second helical shape with a second longitudinal length different from the first longitudinal length of the first microwave resonator, the first and second microwave resonators oppositely handed with respect to each other; and

a coplanar waveguide resonator disposed on an exterior of the tubular;

generating, by the first microwave resonator, a first electric field that rotates along the first helical shape of the first microwave resonator;

generating, by the second microwave resonator, a second electric field that rotates along the second helical shape of the second microwave resonator;

generating, by the coplanar waveguide resonator, a third electric field; and

determining a fluid characteristic of the multiphase fluid in response to generating the first, second, and third electric fields, the fluid characteristic comprising at least one of flow rate, salinity, or phase fraction.

16. The method of claim 15, wherein the first electric field makes at least a 360 degree rotation along the first helical shape of the first microwave resonator, and the second electric field makes at least a 360 degree rotation along the second helical shape of the second microwave resonator.

17. The method of claim 16, wherein:

the apparatus comprises a first conical end and a second conical end;

the first and second conical ends are coupled to the tubular at opposite ends of the tubular;

the first microwave resonator is disposed on and wraps around an exterior of the first conical end; and

the second microwave resonator is disposed on and wraps around an exterior of the second conical end.

18. The method of claim 16, wherein:

the first and second microwave resonators are disposed on the exterior of the tubular; and

flowing the multiphase fluid to contact the apparatus comprises flowing the multiphase fluid through an inner bore of the tubular.

19. The method of claim 18, comprising:

generating, by a second coplanar waveguide resonator, a fourth electric field; and

determining a dielectric loss of the multiphase fluid in response to generating the third and fourth electric fields.